Slot-coupled CW standing wave accelerating cavity
A slot-coupled CW standing wave multi-cell accelerating cavity. To achieve high efficiency graded beta acceleration, each cell in the multi-cell cavity may include different cell lengths. Alternatively, to achieve high efficiency with acceleration for particles with beta equal to 1, each cell in the multi-cell cavity may include the same cell design. Coupling between the cells is achieved with a plurality of axially aligned kidney-shaped slots on the wall between cells. The slot-coupling method makes the design very compact. The shape of the cell, including the slots and the cone, are optimized to maximize the power efficiency and minimize the peak power density on the surface. The slots are non-resonant, thereby enabling shorter slots and less power loss.
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This application claims the priority of Provisional U.S. Patent Application Ser. No. 62/011,920 filed Jun. 13, 2014.
GOVERNMENT LICENSE RIGHTSThis invention was made with government support under Management and Operating Contract No. DE-ACO5-060R23177 awarded by the Department of Energy. The United States Government has certain rights in the invention.
FIELD OF THE INVENTIONThe present invention relates to particle accelerator structures and more particularly to a continuous wave (CW) multi-cell accelerating cavity.
BACKGROUND OF THE INVENTIONThe side-coupling arrangement used in conventional accelerator cavities results in a large and complex assembly. Injectors using cavities of this type combined with thermionic cathodes typically exhibit an electron capture efficiency of less than 40%.
In order to reduce the performance limitations of side-coupled cavities, resonant coupling slots have been proposed in multi-cell accelerator structures. However, resonant slots require long slot openings and lead to high power losses and reduced efficiency.
This is important for industrial or medical applications requiring high average power beams. Unlike pulsed accelerators, where the thermal issues are less important, this invention is aimed at CW and high duty factor applications with high average beam power. The inclusion of the internal cooling is important in this regard and yields an additional advantage
Accordingly, it would be desirable to provide a more compact and simpler accelerator arrangement and method for increasing the electron capture efficiency. Improving the power efficiency of the accelerating structure and the electron capture efficiency leads to a more compact and cost effective device and reduces the amount of input power required to drive the accelerator. This is particularly important for Continuous wave (CW) and high duty factor accelerators where the input power and cooling requirements are significant.
OBJECT OF THE INVENTIONIt is therefore an object of the present invention to provide a more compact and simpler accelerator arrangement for a particle accelerator.
A further object of the invention is to provide a method for increasing the electron capture efficiency a particle accelerator.
Another object of the invention is to provide an accelerator arrangement that reduces the amount of input power required to drive the accelerator for a given output energy.
A further object is to provide an accelerator arrangement for Continuous Wave (CW) and high duty-factor accelerators that significantly reduces the input power and cooling requirements.
A further object of the invention is to provide cavities with internal slots that are symmetrical with respect to the cavity center axis and which do not introduce any transverse kicks to the accelerating beam and allow higher current operation.
BRIEF SUMMARY OF THE INVENTIONThe present invention is a compact, efficient CW standing wave multi-cell accelerating cavity. To achieve high electron capture efficiency a graded beta accelerating structure is used in which each cell in the multi-cell cavity may have different cell lengths. Alternatively, to achieve high efficiency of acceleration for particles with beta equal to 1 (i.e. already traveling close to the speed of light), each cell in the multi-cell cavity may have the same optimized cell design. The coupling between cells is realized with a plurality of kidney-shaped slots on the wall between cells. The slot-coupling method makes the design very compact. The shape of the cell, including the slots and the cone, are optimized to maximize the power efficiency and minimize the peak power density on the surface. The slots are non-resonant, thereby enabling shorter slot lengths and less power loss.
The present invention is a compact, efficient CW standing wave accelerating cavity. This is a multi-cell cavity that can be used for graded beta acceleration with different cell designs, or for beta equal to 1 acceleration with the same cell design for each single cell. The coupling between cells is realized with a plurality of kidney-shaped slots on the wall between cells. The slot-coupling method makes the design very compact. The shape of the cell, including the slots and the cone, are optimized to maximize the power efficiency and minimize the peak power density on the surface.
Referring to
With reference to
For operation in CW mode, the cooling is important. As shown in the left portion of
With reference to
Referring to
With reference to
The bounding box of the CEBAF capture cavity at Jefferson National Accelerator Facility, Newport News, Virginia, has a transverse dimension of 14.3×30 cm2. In a compact, efficient CW standing wave accelerating cavity with a slot-coupling arrangement according to the present invention, the bounding box has a transverse dimension of 13.4×13.4 cm2. Much less power is required to achieve same acceleration results; 7 kW is needed for the slot-coupling design, versus approximately 10 kW in the traditional side-coupling design. The shunt impedance of the new slot-coupling design is 22 MOhm/m, as compared to larger than 18.8 MOhm/m in the side-coupling design.
As a comparison with conventional side-coupling design accelerators, the electron capture efficiency of Varian's 600C, available from Varian Medical Systems, Inc., Palo Alto, Calif., is 37%, while the slot-coupling design provides nearly 100% capture efficiency. After being scaled to 2998 MHz, the slot-coupling design has a shunt impedance of 151 MOhm/m, as compared with 115 MOhm in the Varian 600C.
As a further comparison, the cavities at LEP (Large Electron-Positron Collider at CERN in Geneva, Switzerland) and PEP (SLAC National Accelerator Laboratory at Stanford University, Palo Alto, Calif.) used two-slot coupling for pill-box shaped cells. They operate at about 352 MHz. After being scaled to 352 MHz, the slot-coupling design of the present invention with better cell shape has a higher shunt impedance of 31 MOhm/m, as compared with 26 MOhm/m (LEP) and 21 MOhm/m (PEP).
The compact and axis-symmetric nature of the new structure greatly simplifies embedding in a solenoid magnet for focusing or for transporting magnetized beams. In the present invention, the slots are non-resonant, thereby enabling shorter slot lengths and less power loss. The symmetry of the interior slots about the central axis of the cavities does not introduce any transverse (dipole) kicks, as compared to prior art multi-cell accelerator cavities having resonant slots. In cavities with resonant slots, transverse kicks are produced and must be averaged out by flipping the slot from one side to the other in alternate cells. The symmetry allows the propagation and extraction (damping) of all unwanted transverse higher-order modes (HOMs) that can cause beam break-up instabilities. This allows higher beam current to be operated stably. This is not possible with prior art one- or two-slot designs.
The description of the present invention has been presented for purposes of illustration and description, but is not intended to be exhaustive or limited to the invention in the form disclosed. Many modifications and variations will be apparent to those of ordinary skill in the art without departing from the scope and spirit of the invention. The embodiments herein were chosen and described in order to best explain the principles of the invention and the practical application, and to enable others of ordinary skill in the art to understand the invention for various embodiments with various modifications as are suited to the particular use contemplated.
Claims
1. A slot-coupled continuous wave (CW) graded beta standing wave accelerating cavity, comprising:
- a plurality of interconnected cells including a gap spacing, a cell length, a cone having a cone angle, a center bore, and a center axis extending longitudinally through the center bore;
- a wall between each of said interconnected cells;
- a plurality of non resonant coupling slots on the walls between said interconnected cells;
- said coupling slots in said walls are in axial alignment with a corresponding slot in the plurality of interconnected cells and are offset to a common side from the center axis of the accelerating cavity;
- the plurality of interconnected cells including a gap spacing and cell length that are varied throughout the length of the interconnected cells to accommodate varying beta and the cone angle is constant throughout the length of the interconnected cells;
- the interconnected cells include a center symmetric axis and the slots in each wall are axisymmetric about the center axis; and
- each of said coupling slots extends no more than an angle of 60 degrees around the center symmetric axis.
2. The slot-coupled CW standing wave accelerating cavity of claim 1, further comprising
- an equator on each of said cells; and
- a cylindrical strip at each equator.
3. The slot-coupled CW standing wave accelerating cavity of claim 1, wherein said slots are kidney-shaped.
4. The slot-coupled CW standing wave accelerating cavity of claim 1, further comprising three or more of said slots on each of said walls.
5. The slot-coupled CW standing wave accelerating cavity of claim 2, wherein each of said cells in said plurality of interconnected cells is of a different length for graded beta acceleration.
6. The slot-coupled CW standing wave accelerating cavity of claim 5, wherein the width of the cylindrical strip is changed for different cells to vary the cell length.
7. The slot-coupled CW standing wave accelerating cavity of claim 1, wherein
- the plurality of cells include a gap spacing and a cell length;
- the plurality of cells form a graded beta cavity; and
- the gap spacing and cell length are varied to accommodate varying beta and form a graded beta cavity.
8. The slot-coupled CW standing wave accelerating cavity of claim 7, wherein
- each of the interconnected cells in the plurality of cells include a cone angle; and
- the cone angle is same for all cells.
9. The slot-coupled CW standing wave accelerating cavity of claim 1, wherein each of said cells in said plurality of interconnected cells is of equal lengths for beta equal to 1 acceleration.
10. The slot-coupled CW standing wave accelerating cavity of claim 1, further comprising an internal cooling channel in each wall.
11. The slot-coupled CW standing wave accelerating cavity of claim 1, wherein the dimensions and geometry for the cell walls and slots are the same in each cell.
12. A method for high efficiency continuous wave (CW) graded beta acceleration, comprising:
- a. providing a particle accelerator including a plurality of interconnected cells of varying length separated by walls there between, the interconnected cells including a center symmetric axis, a gap spacing, a cell length, and a cone having a cone angle;
- b. providing a plurality of non resonant coupling slots on the walls between the interconnected cells to enable a pi-mode oscillating field;
- c. axially aligning the coupling slots in the walls along an axis parallel with and offset to a common side from the center symmetric axis;
- d. varying the gap spacing and cell length throughout the length of the interconnected cells to accommodate varying beta;
- e. maintaining a constant cone angle throughout the interconnected cells; and
- f. limiting the extent of each of said coupling slots to no more than an angle of 60 degrees around the center symmetric axis.
13. The method of claim 12, further comprising
- providing a gap spacing between the interconnected cells; and
- varying the gap spacing between the cells accommodate varying beta and form a graded beta cavity.
14. The method of claim 12, further comprising providing an internal cooling channel in each wall.
15. The method of claim 12, further comprising
- providing a cone having a cone angle on each of said cells; and
- setting the cone angle the same for all cells.
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Type: Grant
Filed: Jun 5, 2015
Date of Patent: May 16, 2017
Patent Publication Number: 20150366046
Assignee: JEFFERSON SCIENCE ASSOCIATES, LLC (Newport News, VA)
Inventors: Shaoheng Wang (Yorktown, VA), Robert Rimmer (Yorktown, VA), Haipeng Wang (Glen Allen, VA)
Primary Examiner: Douglas W Owens
Assistant Examiner: Srinivas Sathiraju
Application Number: 14/731,887
International Classification: H05H 7/22 (20060101); H05H 9/04 (20060101); H05H 7/18 (20060101);